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1 - 10 of 20 search results for KaKaoTalk:vb20 200 |u:www-g.eng.cam.ac.uk where 0 match all words and 20 match some words.

  1. Results that match 1 of 2 words

  2. Symmetric prismatic tensegrity structures: Part I. Configuration and…

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009GuestD.pdf
    6 Feb 2014: Higher-Order Rigidity – What Is the Proper Definition. Discrete & Computational Geometry 11, 193–200.Connelly, R., Terrell, M., 1995.

  3. STu1N.8.pdf CLEO:2014 © 2014 OSA Sub-50 fs compressed pulses ...

    www-g.eng.cam.ac.uk/nms/publications/pdf/STu1N.8.pdf
    10 Jun 2014: 1500 1525 1550 1575 1600 1625. -40. -20. 0. -600 -400 -200 0 200 400 600.

  4. STu1I.2.pdf CLEO:2014 © 2014 OSA Synchronously coupled fiber lasers…

    www-g.eng.cam.ac.uk/nms/publications/pdf/STu1I.2.pdf
    10 Jun 2014: Express 20, 25077 (2012).8. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.

  5. STh3N.8.pdf CLEO:2014 © 2014 OSA Nanotube mode-locked, low repetition …

    www-g.eng.cam.ac.uk/nms/publications/pdf/STh3N.8.pdf
    10 Jun 2014: Express21, 23261 (2013).10. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.

  6. RAPID COMMUNICATIONS PHYSICAL REVIEW B 89, 121402(R) (2014) Effects…

    www-g.eng.cam.ac.uk/nms/publications/pdf/PhysRevB.89.121402.pdf
    6 Mar 2014: 200 K. 230 K260 K. 1300120011001000. Raman Shift (cm-1. ). 30 T(b) (1,1). ... Vunit. l3B. 2B. γ 21. 2v. V1B 4.1 106 cm1. This value leads to W (kz) 104 cm1 at 30 T and 200 K,too small to explain the observed

  7. Photodetectors based on graphene, other two-dimensional materials and …

    www-g.eng.cam.ac.uk/nms/publications/pdf/nnano.2014.215.pdf
    6 Oct 2014: Because the optical phonon energy in graphene is large45,46 (200  meV), hot carriers created by the radiation field can remain at a tempera-ture Te (and thus energy kBTe, with ... 100. –200. –300. –400. –500. Phot. ocur. rent. (nA. ). Gate

  8. Numerical analysis of morphing corrugated plates

    www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2009Procedia.pdf
    3 Feb 2014: 5. 6. 7. θ [rad]. m/D. κ T0. φ = 43o, t = 0.2 mmL = 200 mmL = 300 mmL = 400 mmL = 500 mm. ... Gentilini C. et al./ Physics Engineering 01 (2009) 000–000. 200 250 300 350 400 450 500.

  9. nl400516a 1..6

    www-g.eng.cam.ac.uk/nms/publications/pdf/nl400516a.pdf
    4 Sep 2014: sweeping both top gates simultaneously at a drain-sourcevoltage VD = 200 mV. ... b) Electrical transfer characteristics of a 1L-MoS2 FET at biasvoltage VD = 200 mV.

  10. Luminsescence: The Instrumental Key to the Future of Nanotechnology

    www-g.eng.cam.ac.uk/nms/publications/pdf/Acf_Ch06_2014.pdf
    5 Mar 2014: In the 1,200–1,350 nm emission range, exciton-exciton resonances of SWNTs such as (13,2), (12,4), (10,5), (9,7), (10,6), (8,7), (11,4), ... 6.4a) with respect to other tubes. The strong PL emission in the 1,080–1,200 nm range.

  11. JTu4A.67.pdf CLEO:2014 © 2014 OSA Graphene saturable absorber power…

    www-g.eng.cam.ac.uk/nms/publications/pdf/JTu4A.67.pdf
    10 Jun 2014: 0.0. 0.2. 0.4. 0.6. 0.8. 1.0. 0 50 100 150 200 250 300 3500. ... Commun. 4, 1987, (2013).7. D. Popa, et al., “Sub 200 fs pulse generation from a graphene mode-locked fiber laser,” Appl.

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